Camera optical lens

ABSTRACT

The present disclosure provides a camera optical lens. The camera optical lens includes, from an object side to an image side: an aperture; a first lens having a positive refractive power; a second lens having a negative refractive power; a third lens having a positive refractive power; a fourth lens having a negative refractive power; a fifth lens having a positive refractive power; a sixth lens having a negative refractive power; and a seventh lens having a negative refractive power. The camera optical lens satisfies following conditions: 9.00≤f3/f≤30.00; and 2.90≤v1/v2≤5.00, where f denotes a focal length of the camera optical lens; f3 denotes a focal length of the third lens; v1 denotes an abbe number of the first lens; and v2 denotes an abbe number of the second lens.

TECHNICAL FIELD

The present disclosure relates to the field of optical lens, and more particularly, to a camera optical lens suitable for handheld terminal devices such as smart phones or digital cameras and camera devices such as monitors or PC lenses.

BACKGROUND

With the emergence of smart phones in recent years, the demand for miniature camera lens is increasing day by day, but in general the photosensitive devices of camera lens are nothing more than Charge Coupled Device (CCD) or Complementary Metal-Oxide Semiconductor Sensor (CMOS sensor), and as the progress of the semiconductor manufacturing technology makes the pixel size of the photosensitive devices become smaller, plus the current development trend of electronic products towards better functions and thinner and smaller dimensions, miniature camera lenses with good imaging quality therefore have become a mainstream in the market.

In order to obtain better imaging quality, the lens that is traditionally equipped in mobile phone cameras adopts a three-piece or four-piece lens structure, or even five-piece or six piece lens structure. Also, with the development of technology and the increase of the diverse demands of users, and as the pixel area of photosensitive devices is becoming smaller and smaller and the requirement of the system on the imaging quality is improving constantly, a seven-piece lens structure gradually appears in lens designs. Although the common seven-piece lens has good optical performance, its settings on refractive power, lens spacing and lens shape still have some irrationality, which results in that the lens structure cannot achieve a high optical performance while satisfying design requirements of ultra-thin lenses having a big aperture.

BRIEF DESCRIPTION OF DRAWINGS

Many aspects of the exemplary embodiment can be better understood with reference to the following drawings. The components in the drawings are not necessarily drawn to scale, the emphasis instead being placed upon clearly illustrating the principles of the present disclosure. Moreover, in the drawings, like reference numerals designate corresponding parts throughout the several views.

FIG. 1 is a schematic diagram of a structure of a camera optical lens in accordance with Embodiment 1 of the present disclosure;

FIG. 2 is a schematic diagram of a longitudinal aberration of the camera optical lens shown in FIG. 1;

FIG. 3 is a schematic diagram of a lateral color of the camera optical lens shown in FIG. 1;

FIG. 4 is a schematic diagram of a field curvature and a distortion of the camera optical lens shown in FIG. 1;

FIG. 5 is a schematic diagram of a structure of a camera optical lens in accordance with Embodiment 2 of the present disclosure;

FIG. 6 is a schematic diagram of a longitudinal aberration of the camera optical lens shown in FIG. 5;

FIG. 7 is a schematic diagram of a lateral color of the camera optical lens shown in FIG. 5;

FIG. 8 is a schematic diagram of a field curvature and a distortion of the camera optical lens shown in FIG. 5;

FIG. 9 is a schematic diagram of a structure of a camera optical lens in accordance with Embodiment 3 of the present disclosure;

FIG. 10 is a schematic diagram of a longitudinal aberration of the camera optical lens shown in FIG. 9;

FIG. 11 is a schematic diagram of a lateral color of the camera optical lens shown in FIG. 9; and

FIG. 12 is a schematic diagram of a field curvature and a distortion of the camera optical lens shown in FIG. 9;

FIG. 13 is a schematic diagram of a structure of a camera optical lens in accordance with Embodiment 4 of the present disclosure;

FIG. 14 is a schematic diagram of a longitudinal aberration of the camera optical lens shown in FIG. 13;

FIG. 15 is a schematic diagram of a lateral color of the camera optical lens shown in FIG. 13; and

FIG. 16 is a schematic diagram of a field curvature and a distortion of the camera optical lens shown in FIG. 13.

DESCRIPTION OF EMBODIMENTS

The present disclosure will hereinafter be described in detail with reference to several exemplary embodiments. To make the technical problems to be solved, technical solutions and beneficial effects of the present disclosure more apparent, the present disclosure is described in further detail together with the figure and the embodiments. It should be understood the specific embodiments described hereby is only to explain the disclosure, not intended to limit the disclosure.

Embodiment 1

Referring to FIG. 1, the present disclosure provides a camera optical lens 10. FIG. 1 shows the camera optical lens 10 according to Embodiment 1 of the present disclosure. The camera optical lens 10 includes 7 lenses. Specifically, the camera optical lens 10 includes, from an object side to an image side, an aperture S1, a first lens L1, a second lens L2, a third lens L3, a fourth lens L4, a fifth lens L5, a sixth lens L6 and a seventh lens L7. In this embodiment, preferably, an optical element such as a glass plate GF can be arranged between the seventh lens L7 and an image plane Si. The glass plate GF can be a glass cover plate or an optical filter. In other embodiments, the glass plate GF can also be arranged at other positions.

In this embodiment, the first lens L1 has a positive refractive power, and has an object side surface being a convex surface and an image side surface being a concave surface; the second lens L2 has a negative refractive power, and has an object side surface being a convex surface and an image side surface being a concave surface; the third lens L3 has a positive refractive power, and has an object side surface being a concave surface and an image side surface being a convex surface; the fourth lens L4 has a negative refractive power, and has an object side surface being a convex surface and an image side surface being a concave surface; the fifth lens L5 has a positive refractive power, and has an object side surface being a concave surface and an image side surface being a convex surface; the sixth lens L6 has a negative refractive power, and has an object side surface being a concave surface and an image side surface being a concave surface; and the seventh lens L7 has a negative refractive power, and has an object side surface being a concave surface and an image side surface being a concave surface.

Here, a focal length of the camera optical lens 10 is defined as f in a unit of millimeter (mm), a focal length of the third lens L3 is defined as f3, an abbe number of the first lens L1 is defined as v1, and an abbe number of the second lens L2 is defined as v2. The camera optical lens 10 should satisfy satisfies following conditions: 9.00≤f3/f≤30.00  (1); and 2.90≤v1/v2≤5.00  (2).

The condition (1) specifies a ratio of the focal length of the third lens L3 and the focal length of the camera optical lens 10. This leads to the appropriate distribution of the refractive power for the third lens L3, such that the field curvature of the system can be effectively balanced for further improving the imaging quality.

The condition (2) specifies a ratio of the abbe number v1 of the first lens L1 and the abbe number v2 of the second lens L2. This facilitates development towards ultra-thin lenses with a big aperture, and also facilitates correction of aberrations.

In this embodiment, with the above configurations of the lenses, the camera optical lens can achieve a high optical performance while satisfying design requirements for ultra-thin lenses having a big aperture.

In an example, a focal length of the second lens L2 is defined as f2. The camera optical lens 10 further satisfies a condition of: −5.00≤f2/f≤−3.00  (3).

The condition (3) specifies a ratio of the focal length of the second lens L2 and the focal length of the camera optical lens 10. This can effectively balance a spherical aberration caused by the first lens and the field curvature of the system.

In an example, an on-axis thickness of the second lens L2 is defined as d3, an on-axis thickness of the third lens L3 is defined as d5, and a total optical length from the object side surface of the first lens L1 to the image plane of the camera optical lens 10 along an optic axis is defined as TTL. The camera optical lens 10 further satisfies a condition of: 0≤(d3+d5)/TTL≤0.10  (4).

The condition (4) specifies a ratio of a sum of the on-axis thicknesses of the second lens L2 and the third lens L3 and the TTL. This can facilitate improving the image quality while achieving ultra-thin lenses.

In an example, a curvature radius of the object side surface of the third lens L3 is defined as R5, and a curvature radius of the image side surface of the third lens L3 is defined as R6. The camera optical lens 10 further satisfies a condition of: 4.00≤(R5+R6)/(R5−R6)≤11.00  (5).

The condition (5) specifies a shape of the third lens L3. This can facilitate shaping of the third lens L3 and avoid bad shaping and generation of stress due to the overly large surface curvature of the third lens L3.

In an example, a curvature radius of the object side surface of the fourth lens L4 is defined as R7, and a curvature radius of the image side surface of the fourth lens L4 is defined as R8. The camera optical lens 10 further satisfies a condition of: 5.00≤(R7+R8)/(R7−R8)≤20.00  (6).

The condition (6) specifies a shape of the third lens L4. This can facilitate correcting an off-axis aberration.

In this embodiment, the first lens L1 is made of a glass material, and thus the first lens L1 has a good performance in terms of temperature and humidity reliability and has a large Abbe number, thereby effectively correcting a chromatic aberration while improving the optical performance of the camera optical lens. In this embodiment, each of the second lens L2, the third lens L3, the fourth lens L4, the fifth lens L5, the sixth lens L6 and the seventh lens L7 is made of a plastic material. This can effectively reduce production costs.

In addition, a surface of a lens can be set as an aspherical surface. The aspherical surface can be easily formed into a shape other than the spherical surface, so that more control variables can be obtained to reduce the aberration, thereby reducing the number of lenses and thus effectively reducing a total length of the camera optical lens according to the present disclosure. In an embodiment of the present disclosure, both an object side surface and an image side surface of each lens are aspherical surfaces.

It should be noted that the first lens L1, the second lens L2, the third lens L3, the fourth lens L4, the fifth lens L5, the sixth lens L6 and the seventh lens L7 that constitute the camera optical lens 10 of the present embodiment have the structure and parameter relationships as described above, and therefore, the camera optical lens 10 can reasonably distribute the refractive power, the surface shape, the material, the on-axis thickness and the like of each lens, and thus correct various aberrations. The camera optical lens 10 has Fno≤1.45. TTL and an image height (IH) of the camera optical lens 10 satisfy a condition of TTL/IH≤1.48. The field of view (FOV) of the camera optical lens 10 satisfies FOV≥76 degrees. This can achieve a high optical performance while satisfying design requirements for ultra-thin lenses having a big aperture.

In an example, inflexion points and/or arrest points can be arranged on the object side surface and/or image side surface of the lens, so as to satisfy the demand for the high quality imaging. The description below can be referred to for specific implementations.

The design information of the camera optical lens 10 in Embodiment 1 of the present disclosure is shown in the following. It should be noted that each of the distance, radii and the thickness is in a unit of millimeter (mm).

Table 1 and Table 2 show design data of the camera optical lens 10 according to Embodiment 1 of the present disclosure.

TABLE 1 R d nd νd S1 ∞ d0= −0.634 R1 1.987 d1= 1.158 nd1 1.5378 ν1 74.70 R2 10.351 d2= 0.041 R3 9.233 d3= 0.222 nd2 1.6610 ν2 20.53 R4 4.849 d4= 0.489 R5 −18.701 d5= 0.221 nd3 1.6610 ν3 20.53 R6 −15.332 d6= 0.076 R7 6.169 d7= 0.333 nd4 1.5444 ν4 55.82 R8 5.411 d8= 0.468 R9 −13.995 d9= 0.465 nd5 1.5444 ν5 55.82 R10 −1.774 d10= 0.045 R11 −23.288 d11= 0.313 nd6 1.6610 ν6 20.53 R12 12.810 d12= 0.487 R13 −3.636 d13= 0.296 nd7 1.5444 ν7 55.82 R14 4.461 d14= 0.625 R15 ∞ d15= 0.210 ndg 1.5168 νg 64.17 R16 ∞ d16= 0.140

In the table, meanings of various symbols will be described as follows.

S1: aperture;

R: curvature radius of an optical surface, a central curvature radius for a lens;

R1: curvature radius of the object side surface of the first lens L1;

R2: curvature radius of the image side surface of the first lens L1;

R3: curvature radius of the object side surface of the second lens L2;

R4: curvature radius of the image side surface of the second lens L2;

R5: curvature radius of the object side surface of the third lens L3;

R6: curvature radius of the image side surface of the third lens L3;

R7: curvature radius of the object side surface of the fourth lens L4;

R8: curvature radius of the image side surface of the fourth lens L4;

R9: curvature radius of the object side surface of the fifth lens L5;

R10: curvature radius of the image side surface of the fifth lens L5;

R11: curvature radius of the object side surface of the sixth lens L6;

R12: curvature radius of the image side surface of the sixth lens L6;

R13: curvature radius of the object side surface of the seventh lens L7;

R14: curvature radius of the image side surface of the seventh lens L7;

R15: curvature radius of an object side surface of the optical filter GF;

R16: curvature radius of an image side surface of the optical filter GF;

d: on-axis thickness of a lens and an on-axis distance between lenses;

d0: on-axis distance from the aperture S1 to the object side surface of the first lens L1;

d1: on-axis thickness of the first lens L1;

d2: on-axis distance from the image side surface of the first lens L1 to the object side surface of the second lens L2;

d3: on-axis thickness of the second lens L2;

d4: on-axis distance from the image side surface of the second lens L2 to the object side surface of the third lens L3;

d5: on-axis thickness of the third lens L3;

d6: on-axis distance from the image side surface of the third lens L3 to the object side surface of the fourth lens L4;

d7: on-axis thickness of the fourth lens L4;

d8: on-axis distance from the image side surface of the fourth lens L4 to the object side surface of the fifth lens L5;

d9: on-axis thickness of the fifth lens L5;

d10: on-axis distance from the image side surface of the fifth lens L5 to the object side surface of the sixth lens L6;

d11: on-axis thickness of the sixth lens L6;

d12: on-axis distance from the image side surface of the sixth lens L6 to the object side surface of the seventh lens L7;

d13: on-axis thickness of the seventh lens L7;

d14: on-axis distance from the image side surface of the seventh lens L7 to the object side surface of the optical filter GF;

d15: on-axis thickness of the optical filter GF;

d16: on-axis distance from the image side surface of the optical filter GF to the image plane;

nd: refractive index of d line;

nd1: refractive index of d line of the first lens L1;

nd2: refractive index of d line of the second lens L2;

nd3: refractive index of d line of the third lens L3;

nd4: refractive index of d line of the fourth lens L4;

nd5: refractive index of d line of the fifth lens L5;

nd6: refractive index of d line of the sixth lens L6;

nd7: refractive index of d line of the seventh lens L7;

ndg: refractive index of d line of the optical filter GF;

vd: abbe number;

v1: abbe number of the first lens L1;

v2: abbe number of the second lens L2;

v3: abbe number of the third lens L3;

v4: abbe number of the fourth lens L4;

v5: abbe number of the fifth lens L5;

v6: abbe number of the sixth lens L6;

v7: abbe number of the seventh lens L7;

vg: abbe number of the optical filter GF.

Table 2 shows aspherical surface data of the camera optical lens 10 in Embodiment 1 of the present disclosure.

TABLE 2 Conic coefficient Aspherical surface coefficients k A4 A6 A8 A10 R1 −4.8349E−01 −1.0740E−03   1.3185E−02 −1.6884E−02   1.1653E−02 R2 −5.1855E+00 1.2620E−01 −3.6881E−01 4.3075E−01 −2.8472E−01 R3  3.7046E+01 1.6401E−01 −4.1108E−01 5.1146E−01 −3.7999E−01 R4  1.1691E+01 8.4524E−02 −1.8794E−01 3.4580E−01 −4.4857E−01 R5  1.7926E+02 1.2591E−01 −3.6931E−01 6.1843E−01 −6.6714E−01 R6  1.0664E+02 2.3960E−01 −8.1613E−01 1.5771E+00 −1.9075E+00 R7  0.0000E+00 1.1382E−01 −6.0162E−01 1.0251E+00 −9.6662E−01 R8  0.0000E+00 −2.4482E−02  −8.4377E−02 7.4285E−02 −1.0470E−02 R9 −6.7905E+02 −6.1862E−02   2.1789E−01 −2.8306E−01   1.9366E−01 R10 −8.5294E+00 4.4937E−02  2.8091E−02 −1.2438E−01   1.2797E−01 R11 −2.3737E+03 2.4070E−01 −3.1441E−01 1.7152E−01 −5.2787E−02 R12 −9.2371E+02 1.6834E−01 −2.1225E−01 1.1275E−01 −3.8237E−02 R13  1.2857E−01 −4.7255E−03  −7.1033E−02 5.0947E−02 −1.5839E−02 R14 −7.3541E+00 −8.4277E−02   1.2422E−02 2.2961E−03 −9.3880E−04 Aspherical surface coefficients A12 A14 A16 A18 A20 R1 −4.5904E−03   7.7578E−04 −4.3541E−05  0.0000E+00 0.0000E+00 R2 1.0963E−01 −2.2988E−02 2.0287E−03 0.0000E+00 0.0000E+00 R3 1.8182E−01 −5.1476E−02 6.6397E−03 0.0000E+00 0.0000E+00 R4 3.7940E−01 −1.7749E−01 3.5082E−02 0.0000E+00 0.0000E+00 R5 3.9683E−01 −1.1876E−01 1.4189E−02 0.0000E+00 0.0000E+00 R6 1.4128E+00 −6.3839E−01 1.6628E−01 −1.9357E−02  0.0000E+00 R7 5.0076E−01 −1.3173E−01 1.3722E−02 0.0000E+00 0.0000E+00 R8 −2.9114E−02   2.1203E−02 −5.6135E−03  5.2209E−04 0.0000E+00 R9 −7.7314E−02   1.6351E−02 −1.4021E−03  0.0000E+00 0.0000E+00 R10 −7.0388E−02   2.1671E−02 −3.4839E−03  2.2720E−04 0.0000E+00 R11 5.2522E−03  1.4204E−03 −4.0769E−04  2.8923E−05 0.0000E+00 R12 8.1213E−03 −1.0177E−03 6.9217E−05 −2.0213E−06  0.0000E+00 R13 2.7512E−03 −2.7861E−04 1.5464E−05 −3.6474E−07  0.0000E+00 R14 7.9039E−05  5.1689E−06 −1.1658E−06  5.1389E−08 0.0000E+00

Here, k is a conic coefficient, and A4, A6, A8, A10, A12, A14 and A16 are aspheric surface coefficients.

IH: Image Height y=(x ² /R)/[1+{1−(k+1)(x ² /R ²)}^(1/2)]+A4x ⁴ +A6x ⁶ +A8x ⁸ +A10x ¹⁰ +A12x ¹² +A14x ¹⁴ +A16x ¹⁶ +A18x ¹⁸ +A20x ²⁰  (7)

For convenience, an aspheric surface of each lens surface uses the aspheric surfaces shown in the above formula (7). However, the present disclosure is not limited to the aspherical polynomials form shown in the formula (7).

Table 3 and Table 4 show design data of inflexion points and arrest points of respective lens in the camera optical lens 10 according to Embodiment 1 of the present disclosure. P1R1 and P1R2 represent the object side surface and the image side surface of the first lens L1, respectively, P2R1 and P2R2 represent the object side surface and the image side surface of the second lens L2, respectively, P3R1 and P3R2 represent the object side surface and the image side surface of the third lens L3, respectively, P4R1 and P4R2 represent the object side surface and the image side surface of the fourth lens L4, respectively, P5R1 and P5R2 represent the object side surface and the image side surface of the fifth lens L5, respectively, P6R1 and P6R2 represent the object side surface and the image side surface of the sixth lens L6, respectively, and P7R1 and P7R2 represent the object side surface and the image side surface of the seventh lens L7, respectively. The data in the column named “inflexion point position” refers to vertical distances from inflexion points arranged on each lens surface to the optic axis of the camera optical lens 10. The data in the column named “arrest point position” refers to vertical distances from arrest points arranged on each lens surface to the optic axis of the camera optical lens 10.

TABLE 3 Number of Inflexion point Inflexion point Inflexion point Inflexion point inflexion points position 1 position 2 position 3 position 4 P1R1 1 1.395 P1R2 1 0.585 P2R1 P2R2 P3R1 2 0.245 0.425 P3R2 4 0.175 0.465 1.195 1.355 P4R1 3 0.495 1.225 1.445 P4R2 3 0.525 1.405 1.595 P5R1 2 0.495 0.875 P5R2 1 1.925 P6R1 3 0.125 0.715 1.765 P6R2 3 0.735 2.005 2.335 P7R1 1 1.485 P7R2 2 0.475 2.795

TABLE 4 Number of Arrest point Arrest point arrest points position 1 position 2 P1R1 P1R2 1 1.065 P2R1 P2R2 P3R1 P3R2 2 0.385 0.525 P4R1 1 0.875 P4R2 1 0.875 P5R1 P5R2 P6R1 2 0.215 0.975 P6R2 1 1.055 P7R1 1 2.765 P7R2 1 0.855

FIG. 2 and FIG. 3 illustrate a longitudinal aberration and a lateral color of light with wavelengths of 470 nm, 510 nm, 555 nm, 610 nm and 650 nm after passing the camera optical lens 10 according to Embodiment 1. FIG. 4 illustrates a field curvature and a distortion of light with a wavelength of 555 nm after passing the camera optical lens 10 according to Embodiment 1, in which a field curvature S is a field curvature in a sagittal direction and T is a field curvature in a tangential direction.

Table 17 shows various values of Embodiments 1, 2, 3 and 4 and values corresponding to parameters which are specified in the above conditions.

As shown in Table 17, Embodiment 1 satisfies the above conditions.

In this embodiment, the entrance pupil diameter of the camera optical lens is 3.299 mm. The image height of 1.0 H is 3.852 mm. The FOV (field of view) in the diagonal direction is 76.98°. Thus, the camera optical lens can achieve a high optical performance while satisfying design requirements for ultra-thin lenses having a big aperture.

Embodiment 2

Embodiment 2 is basically the same as Embodiment 1 and involves symbols having the same meanings as Embodiment 1, and only differences therebetween will be described in the following.

Table 5 and Table 6 show design data of a camera optical lens 20 in Embodiment 2 of the present disclosure.

TABLE 5 R d nd νd S1 ∞ d0= −0.582 R1 2.109 d1= 1.099 nd1 1.5806 ν1 60.08 R2 10.422 d2= 0.038 R3 23.609 d3= 0.220 nd2 1.6610 ν2 20.53 R4 6.419 d4= 0.455 R5 −18.251 d5= 0.292 nd3 1.6610 ν3 20.53 R6 −15.177 d6= 0.068 R7 5.455 d7= 0.419 nd4 1.5444 ν4 55.82 R8 4.934 d8= 0.357 R9 −13.960 d9= 0.503 nd5 1.5444 ν5 55.82 R10 −1.308 d10= 0.044 R11 −10.410 d11= 0.357 nd6 1.6610 ν6 20.53 R12 8.523 d12= 0.427 R13 −3.814 d13= 0.327 nd7 1.5444 ν7 55.82 R14 3.637 d14= 0.625 R15 ∞ d15= 0.210 ndg 1.5168 νg 64.17 R16 ∞ d16= 0.129

Table 6 shows aspherical surface data of each lens of the camera optical lens 20 in Embodiment 2 of the present disclosure.

TABLE 6 Conic coefficient Aspherical surface coefficients k A4 A6 A8 A10 R1 −3.9959E−01 3.0848E−03 1.0432E−02 −1.7580E−02  1.2276E−02 R2 −8.2006E+01 1.2984E−01 −3.6397E−01   4.3000E−01 −2.8538E−01 R3 −3.5955E+01 1.7242E−01 −4.0782E−01   5.1063E−01 −3.8127E−01 R4  5.1236E+00 9.9137E−02 −1.8130E−01   3.4465E−01 −4.5968E−01 R5  1.6990E+02 1.1851E−01 −3.7122E−01   6.2389E−01 −6.6672E−01 R6  6.6229E+01 2.5166E−01 −8.6090E−01   1.5327E+00 −1.6248E+00 R7  0.0000E+00 9.7026E−02 −5.9800E−01   1.0297E+00 −9.6540E−01 R8  0.0000E+00 −6.7254E−02  9.2537E−02 −2.7277E−01  3.6424E−01 R9 −1.0001E+03 −3.7941E−02  2.2056E−01 −2.8339E−01  1.9340E−01 R10 −9.1464E+00 −1.3325E−01  4.0348E−01 −5.2669E−01  4.1110E−01 R11 −1.1126E+03 5.8609E−02 2.9880E−03 −8.8264E−02  7.1807E−02 R12 −1.1655E+02 −4.1526E−02  7.5574E−02 −7.9701E−02  3.6946E−02 R13  1.3165E−02 −8.4922E−02  2.4042E−02  5.3707E−03 −4.4435E−03 R14 −4.2969E+00 −1.1274E−01  4.3025E−02 −1.1566E−02  2.4098E−03 Aspherical surface coefficients A12 A14 A16 A18 A20 R1 −4.3987E−03  7.5584E−04 −7.4020E−05 0.0000E+00 0.0000E+00 R2  1.0927E−01 −2.3083E−02  2.1131E−03 0.0000E+00 0.0000E+00 R3  1.8139E−01 −5.1266E−02  6.4433E−03 0.0000E+00 0.0000E+00 R4  3.8552E−01 −1.7108E−01  3.0560E−02 0.0000E+00 0.0000E+00 R5  3.9663E−01 −1.1848E−01  1.4082E−02 0.0000E+00 0.0000E+00 R6  9.8458E−01 −3.1996E−01  4.7705E−02 −1.8687E−03  0.0000E+00 R7  5.0055E−01 −1.3204E−01  1.3646E−02 0.0000E+00 0.0000E+00 R8 −2.7076E−01  1.1359E−01 −2.4767E−02 2.1661E−03 0.0000E+00 R9 −7.7363E−02  1.6352E−02 −1.4036E−03 0.0000E+00 0.0000E+00 R10 −1.9818E−01  5.6399E−02 −8.6387E−03 5.4856E−04 0.0000E+00 R11 −3.1792E−02  8.1915E−03 −1.1030E−03 5.9338E−05 0.0000E+00 R12 −9.4192E−03  1.3526E−03 −9.9242E−05 2.7470E−06 0.0000E+00 R13  1.1820E−03 −1.6515E−04  1.2073E−05 −3.6432E−07  0.0000E+00 R14 −3.7269E−04  3.7281E−05 −2.0514E−06 4.6368E−08 0.0000E+00

Table 7 and Table 8 show design data of inflexion points and arrest points of respective lens in the camera optical lens 20 according to Embodiment 2 of the present disclosure.

TABLE 7 Number of Inflexion point Inflexion point Inflexion point inflexion points position 1 position 2 position 3 P1R1 1 1.395 P1R2 1 0.585 P2R1 P2R2 P3R1 3 0.295 0.345 1.185 P3R2 3 0.175 0.435 1.185 P4R1 3 0.485 1.185 1.345 P4R2 3 0.545 1.385 1.505 P5R1 2 0.385 1.065 P5R2 3 0.655 1.135 1.875 P6R1 3 0.255 0.745 1.725 P6R2 3 0.665 2.015 2.355 P7R1 2 1.465 2.655 P7R2 3 0.485 2.595 3.015

TABLE 8 Number of Arrest point Arrest point arrest points position 1 position 2 P1R1 1 1.675 P1R2 1 1.075 P2R1 P2R2 P3R1 P3R2 2 0.365 0.485 P4R1 1 0.875 P4R2 1 0.885 P5R1 2 0.615 1.285 P5R2 P6R1 2 0.495 0.895 P6R2 1 0.985 P7R1 2 2.505 2.745 P7R2 1 0.945

FIG. 6 and FIG. 7 illustrate a longitudinal aberration and a lateral color of light with wavelengths of 470 nm, 510 nm, 555 nm, 610 nm and 650 nm after passing the camera optical lens 20 according to Embodiment 2. FIG. 8 illustrates a field curvature and a distortion of light with a wavelength of 555 nm after passing the camera optical lens 20 according to Embodiment 2.

As shown in Table 17, Embodiment 2 satisfies the above conditions.

In this embodiment, the entrance pupil diameter of the camera optical lens is 3.057 mm. The image height of 1.0 H is 3.852 mm. The FOV (field of view) in the diagonal direction is 81.61°. Thus, the camera optical lens can achieve a high optical performance while satisfying design requirements for ultra-thin lenses having a big aperture.

Embodiment 3

Embodiment 3 is basically the same as Embodiment 1 and involves symbols having the same meanings as Embodiment 1, and only differences therebetween will be described in the following.

Table 9 and Table 10 show design data of a camera optical lens 30 in Embodiment 3 of the present disclosure.

TABLE 9 R d nd νd S1 ∞ d0= −0.644 R1 1.937 d1= 1.278 nd1 1.4342 ν1 94.95 R2 22.857 d2= 0.048 R3 6.856 d3= 0.226 nd2 1.6700 ν2 19.39 R4 4.656 d4= 0.372 R5 −18.158 d5= 0.214 nd3 1.6610 ν3 20.53 R6 −10.901 d6= 0.069 R7 5.740 d7= 0.333 nd4 1.5444 ν4 55.82 R8 5.147 d8= 0.377 R9 −6.843 d9= 0.409 nd5 1.5444 ν5 55.82 R10 −2.119 d10= 0.067 R11 6.259 d11= 0.435 nd6 1.6610 ν6 20.53 R12 5.501 d12= 0.589 R13 −3.562 d13= 0.294 nd7 1.5444 ν7 55.82 R14 4.091 d14= 0.525 R15 ∞ d15= 0.210 ndg 1.5168 νg 64.17 R16 ∞ d16= 0.103

Table 10 shows aspherical surface data of each lens of the camera optical lens 30 in Embodiment 3 of the present disclosure.

TABLE 10 Conic coefficient Aspherical surface coefficients k A4 A6 A8 A10 R1 −4.4021E−01  1.4142E−03 1.0279E−02 −1.9388E−02  1.3777E−02 R2  2.2371E+02  1.3773E−01 −3.7850E−01   4.3080E−01 −2.8223E−01 R3  1.8842E+01  1.4868E−01 −4.1047E−01   5.0525E−01 −3.8274E−01 R4  9.2379E+00  7.6352E−02 −2.0747E−01   3.3771E−01 −4.4311E−01 R5 −2.3160E+02  1.4575E−01 −3.7963E−01   6.1044E−01 −6.6998E−01 R6 −2.5341E+01  3.0053E−01 −1.0327E+00   2.0834E+00 −2.6557E+00 R7  0.0000E+00  1.1443E−01 −6.0318E−01   1.0248E+00 −9.6573E−01 R8  0.0000E+00 −4.8990E−02 3.5394E−02 −1.6122E−01  2.4358E−01 R9 −3.3281E+02 −3.2767E−02 2.1687E−01 −2.8412E−01  1.9332E−01 R10 −1.2568E+01 −1.6023E−01 4.3628E−01 −5.2143E−01  3.8058E−01 R11 −3.6238E+02 −5.4745E−03 5.2551E−02 −1.0793E−01  8.6262E−02 R12 −8.4686E+01 −1.1929E−02 6.1263E−03 −4.8317E−03 −2.4977E−03 R13 −1.7407E−01 −1.1079E−01 5.9562E−02 −2.3574E−02  9.2428E−03 R14 −7.2236E+00 −1.1958E−01 5.7196E−02 −2.1480E−02  5.6439E−03 Aspherical surface coefficients A12 A14 A16 A18 A20 R1 −4.2213E−03  3.3743E−04 2.7034E−05 0.0000E+00 0.0000E+00 R2  1.0925E−01 −2.3423E−02 2.1410E−03 0.0000E+00 0.0000E+00 R3  1.8411E−01 −5.0924E−02 6.1229E−03 0.0000E+00 0.0000E+00 R4  3.7956E−01 −1.7743E−01 3.4152E−02 0.0000E+00 0.0000E+00 R5  3.9649E−01 −1.1807E−01 1.5516E−02 0.0000E+00 0.0000E+00 R6  2.0678E+00 −9.8053E−01 2.6638E−01 −3.1829E−02  0.0000E+00 R7  5.0089E−01 −1.3182E−01 1.3605E−02 0.0000E+00 0.0000E+00 R8 −1.9676E−01  8.9223E−02 −2.1333E−02  2.0974E−03 0.0000E+00 R9 −7.7367E−02  1.6357E−02 −1.3931E−03  0.0000E+00 0.0000E+00 R10 −1.7904E−01  5.1454E−02 −8.0894E−03  5.2910E−04 0.0000E+00 R11 −4.1832E−02  1.1622E−02 −1.6364E−03  8.9738E−05 0.0000E+00 R12  2.2059E−03 −6.1667E−04 7.9668E−05 −3.9696E−06  0.0000E+00 R13 −2.4829E−03  3.8690E−04 −3.1751E−05  1.0649E−06 0.0000E+00 R14 −9.2135E−04  8.7018E−05 −4.2880E−06  8.3062E−08 0.0000E+00

Table 11 and Table 12 show design data of inflexion points and arrest points of respective lens in the camera optical lens 30 according to Embodiment 3 of the present disclosure.

TABLE 11 Number of Inflexion point Inflexion point Inflexion point inflexion points position 1 position 2 position 3 P1R1 1 1.465 P1R2 1 0.555 P2R1 P2R2 P3R1 3 0.205 0.565 1.155 P3R2 3 0.185 0.495 1.155 P4R1 1 0.505 P4R2 1 0.555 P5R1 2 0.405 1.015 P5R2 2 0.665 1.075 P6R1 2 0.645 1.695 P6R2 2 0.665 2.035 P7R1 3 1.415 2.385 2.625 P7R2 1 0.445

TABLE 12 Number of Arrest point Arrest point Arrest point arrest points position 1 position 2 position 3 P1R1 P1R2 1 0.895 P2R1 P2R2 P3R1 2 0.415 0.665 P3R2 3 0.435 0.545 1.295 P4R1 1 0.895 P4R2 1 0.895 P5R1 2 0.705 1.195 P5R2 P6R1 1 0.955 P6R2 1 1.125 P7R1 P7R2 1 0.845

FIG. 10 and FIG. 11 illustrate a longitudinal aberration and a lateral color of light with wavelengths of 470 nm, 510 nm, 555 nm, 610 nm and 650 nm after passing the camera optical lens 30 according to Embodiment 3. FIG. 12 illustrates field curvature and distortion of light with a wavelength of 555 nm after passing the camera optical lens 30 according to Embodiment 3.

As shown in Table 17, Embodiment 1 satisfies the above conditions.

In this embodiment, the entrance pupil diameter of the camera optical lens is 3.117 mm. The image height of 1.0H is 3.852 mm. The FOV (field of view) in the diagonal direction is 80.50°. Thus, the camera optical lens has a big aperture and is ultra-thin, while achieving a high optical performance.

Embodiment 4

Embodiment 4 is basically the same as Embodiment 1 and involves symbols having the same meanings as Embodiment 1, and only differences therebetween will be described in the following.

Table 13 and Table 14 show design data of a camera optical lens 40 in Embodiment 2 of the present disclosure.

TABLE 13 R d nd νd S1 ∞ d0= −0.641 R1 2.035 d1= 1.141 nd1 1.5378 ν1 74.70 R2 12.096 d2= 0.049 R3 11.458 d3= 0.203 nd2 1.6610 ν2 20.53 R4 5.536 d4= 0.418 R5 −28.215 d5= 0.157 nd3 1.6610 ν3 20.53 R6 −17.391 d6= 0.089 R7 22.075 d7= 0.438 nd4 1.5444 ν4 55.82 R8 14.744 d8= 0.417 R9 −39.013 d9= 0.453 nd5 1.5444 ν5 55.82 R10 −2.113 d10= 0.020 R11 −96.605 d11= 0.303 nd6 1.6610 ν6 20.53 R12 26.753 d12= 0.516 R13 −3.414 d13= 0.340 nd7 1.5444 ν7 55.82 R14 4.056 d14= 0.625 R15 ∞ d15= 0.210 ndg 1.5168 νg 64.17 R16 ∞ d16= 0.138

Table 14 shows aspherical surface data of each lens of the camera optical lens 40 in Embodiment 4 of the present disclosure.

TABLE 14 Conic coefficient Aspherical surface coefficients k A4 A6 A8 A10 R1 −4.8818E−01 −1.0740E−03   1.3185E−02 −1.6884E−02   1.1653E−02 R2  1.1242E+00 1.2620E−01 −3.6881E−01 4.3075E−01 −2.8472E−01 R3  5.7249E+01 1.6401E−01 −4.1108E−01 5.1146E−01 −3.7999E−01 R4  1.3039E+01 8.4524E−02 −1.8794E−01 3.4580E−01 −4.4857E−01 R5 −1.6613E+02 1.2591E−01 −3.6931E−01 6.1843E−01 −6.6714E−01 R6  9.1686E+01 2.3960E−01 −8.1613E−01 1.5771E+00 −1.9075E+00 R7  0.0000E+00 1.1382E−01 −6.0162E−01 1.0251E+00 −9.6662E−01 R8  0.0000E+00 −2.4482E−02  −8.4377E−02 7.4285E−02 −1.0470E−02 R9  4.7757E+02 −6.1862E−02   2.1789E−01 −2.8306E−01   1.9366E−01 R10 −7.8083E+00 4.4937E−02  2.8091E−02 −1.2438E−01   1.2797E−01 R11 −1.4159E+03 2.4070E−01 −3.1441E−01 1.7152E−01 −5.2787E−02 R12 −9.9474E+01 1.6834E−01 −2.1225E−01 1.1275E−01 −3.8237E−02 R13 −2.0681E−01 −4.7255E−03  −7.1033E−02 5.0947E−02 −1.5839E−02 R14 −8.6290E+00 −8.4277E−02   1.2422E−02 2.2961E−03 −9.3880E−04 Aspherical surface coefficients A12 A14 A16 A18 A20 R1 −4.5904E−03   7.7578E−04 −4.3541E−05  0.0000E+00 0.0000E+00 R2 1.0963E−01 −2.2988E−02 2.0287E−03 0.0000E+00 0.0000E+00 R3 1.8182E−01 −5.1476E−02 6.6397E−03 0.0000E+00 0.0000E+00 R4 3.7940E−01 −1.7749E−01 3.5082E−02 0.0000E+00 0.0000E+00 R5 3.9683E−01 −1.1876E−01 1.4189E−02 0.0000E+00 0.0000E+00 R6 1.4128E+00 −6.3839E−01 1.6628E−01 −1.9357E−02  0.0000E+00 R7 5.0076E−01 −1.3173E−01 1.3722E−02 0.0000E+00 0.0000E+00 R8 −2.9114E−02   2.1203E−02 −5.6135E−03  5.2209E−04 0.0000E+00 R9 −7.7314E−02   1.6351E−02 −1.4021E−03  0.0000E+00 0.0000E+00 R10 −7.0388E−02   2.1671E−02 −3.4839E−03  2.2720E−04 0.0000E+00 R11 5.2522E−03  1.4204E−03 −4.0769E−04  2.8923E−05 0.0000E+00 R12 8.1213E−03 −1.0177E−03 6.9217E−05 −2.0213E−06  0.0000E+00 R13 2.7512E−03 −2.7861E−04 1.5464E−05 −3.6474E−07  0.0000E+00 R14 7.9039E−05  5.1689E−06 −1.1658E−06  5.1389E−08 0.0000E+00

Table 15 and table 16 show design data of inflexion points and arrest points of respective lens in the camera optical lens 40 according to Embodiment 4 of the present disclosure.

TABLE 15 Number of Inflexion point Inflexion point Inflexion point inflexion points position 1 position 2 position 3 P1R1 1 1.385 P1R2 1 0.575 P2R1 P2R2 P3R1 3 0.175 0.515 1.235 P3R2 3 0.165 0.485 1.175 P4R1 2 0.395 1.235 P4R2 2 0.355 1.415 P5R1 2 0.495 0.845 P5R2 1 1.925 P6R1 3 0.065 0.715 1.765 P6R2 2 0.745 2.005 P7R1 1 1.485 P7R2 2 0.485 2.795

TABLE 16 Number of Arrest point Arrest point arrest points position 1 position 2 P1R1 P1R2 1 1.005 P2R1 P2R2 P3R1 2 0.335 0.645 P3R2 2 0.325 0.625 P4R1 1 0.585 P4R2 1 0.575 P5R1 P5R2 P6R1 2 0.105 0.985 P6R2 1 1.065 P7R1 1 2.695 P7R2 1 0.885

FIG. 14 and FIG. 15 illustrate a longitudinal aberration and a lateral color of light with wavelengths of 470 nm, 510 nm, 555 nm, 610 nm and 650 nm after passing the camera optical lens 240 according to Embodiment 4. FIG. 16 illustrates a field curvature and a distortion of light with a wavelength of 555 nm after passing the camera optical lens 40 according to Embodiment 4.

As shown in Table 17, Embodiment 4 satisfies the above conditions.

In this embodiment, the entrance pupil diameter of the camera optical lens is 3.171 mm. The image height of 1.0 H is 3.852 mm. The FOV (field of view) in the diagonal direction is 79.47°. Thus, the camera optical lens can achieve a high optical performance while satisfying design requirements for ultra-thin lenses having a big aperture.

TABLE 17 Conditions Embodiment 1 Embodiment 2 Embodiment 3 Embodiment 4 Notes f3/f 26.18 29.58 9.01 14.80 Condition (1) v1/v2 3.64 2.93 4.90 3.64 Condition (2) f2/f −3.29 −3.02 −4.99 −3.57 Condition (3) (d3 + d5)/TTL 0.08 0.09 0.08 0.07 Condition (4) (R5 + R6)/(R5 − R6) 10.10 10.87 4.00 4.21 Condition (5) (R7 + R8)/(R7 − R8) 15.28 19.94 18.36 5.02 Condition (6) f 4.750 4.402 4.488 4.567 f1 4.351 4.328 4.776 4.366 f2 −15.637 −13.291 −22.377 −16.286 f3 124.354 130.199 40.436 67.595 f4 −95.387 −131.975 −113.889 −83.048 f5 3.671 2.606 5.372 4.073 f6 −12.352 −6.976 −88.444 −31.392 f7 −3.621 −3.357 −3.440 −3.341 f12 5.442 5.746 5.613 5.442 TTL 5.589 5.570 5.549 5.517

It can be appreciated by one having ordinary skill in the art that the description above is only embodiments of the present disclosure. In practice, one having ordinary skill in the art can make various modifications to these embodiments in forms and details without departing from the spirit and scope of the present disclosure. 

What is claimed is:
 1. A camera optical lens, comprising, from an object side to an image side: an aperture; a first lens having a positive refractive power; a second lens having a negative refractive power; a third lens having a positive refractive power; a fourth lens having a negative refractive power; a fifth lens having a positive refractive power; a sixth lens having a negative refractive power; and a seventh lens having a negative refractive power, wherein the camera optical lens satisfies following conditions: 9.00≤f3/f≤30.00; and 2.90≤v1/v2≤5.00, where f denotes a focal length of the camera optical lens; f3 denotes a focal length of the third lens; v1 denotes an abbe number of the first lens; and v2 denotes an abbe number of the second lens.
 2. The camera optical lens as described in claim 1, further satisfying a following condition: −5.00≤f2/f≤−3.00, where f2 denotes a focal length of the second lens.
 3. The camera optical lens as described in claim 1, further satisfying a following condition: 0≤(d3+d5)/TTL≤0.10, where d3 denotes an on-axis thickness of the second lens; d5 denotes an on-axis thickness of the third lens; and TTL denotes a total optical length from an object side surface of the first lens to an image plane of the camera optical lens along an optic axis.
 4. The camera optical lens as described in claim 1, further satisfying a following condition: 4.00≤(R5+R6)/(R5−R6)≤11.00, where R5 denotes a curvature radius of an object side surface of the third lens; and R6 denotes a curvature radius of an image side surface of the third lens.
 5. The camera optical lens as described in claim 1, further satisfying a following condition: 5.00≤(R7+R8)/(R7−R8)≤20.00, where R7 denotes a curvature radius of an object side surface of the fourth lens; and R8 denotes a curvature radius of an image side surface of the fourth lens. 